source: trunk/source/processes/electromagnetic/lowenergy/include/G4PenelopeCompton.hh @ 1315

Last change on this file since 1315 was 1315, checked in by garnier, 14 years ago

update geant4-09-04-beta-cand-01 interfaces-V09-03-09 vis-V09-03-08

File size: 4.7 KB
Line 
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25//
26// $Id: G4PenelopeCompton.hh,v 1.11 2008/03/26 15:30:19 pandola Exp $
27// GEANT4 tag $Name: geant4-09-04-beta-cand-01 $
28//
29// Author: Luciano Pandola
30//
31// History:
32// -----------
33// 05 Dec 2002   L. Pandola   1st implementation
34// 12 Feb 2003   MG Pia       const argument in SelectRandomAtomForCompton
35// 14 Feb 2003   MG Pia       Modified some variables to lowercase initial
36// 26 Mar 2003   L.Pandola    Added fluorescence
37// 18 Mar 2004   L.Pandola    Use of std::map (code review)
38// 26 Mar 2008   L.Pandola    Add boolean flag to control atomic de-excitation
39//
40// -------------------------------------------------------------------
41
42// Class description:
43// Low Energy Electromagnetic Physics, Compton Scattering
44// Penelope Model
45// -------------------------------------------------------------------
46
47#ifndef G4PENELOPECOMPTON_HH
48#define G4PENELOPECOMPTON_HH 1
49
50#include "globals.hh"
51#include "G4VDiscreteProcess.hh"
52
53class G4Track;
54class G4Step;
55class G4ParticleDefinition;
56class G4VParticleChange;
57class G4VEMDataSet;
58class G4VRangeTest;
59class G4Material;
60
61class G4PenelopeCompton : public G4VDiscreteProcess {
62
63public:
64 
65  G4PenelopeCompton(const G4String& processName ="PenCompton");
66 
67  ~G4PenelopeCompton();
68
69  G4bool IsApplicable(const G4ParticleDefinition& definition);
70 
71  void BuildPhysicsTable(const G4ParticleDefinition& photon);
72 
73  G4VParticleChange* PostStepDoIt(const G4Track& aTrack, const G4Step& aStep);
74 
75  // For testing purpose only
76  G4double DumpMeanFreePath(const G4Track& aTrack, 
77                            G4double previousStepSize, 
78                            G4ForceCondition* condition) 
79  { return GetMeanFreePath(aTrack, previousStepSize, condition); }
80
81  void SetUseAtomicDeexcitation(G4bool value){fUseAtomicDeexcitation = value;};
82
83  G4bool GetUseAtomicDeexcitation(){return fUseAtomicDeexcitation;};
84
85protected:
86
87  G4double GetMeanFreePath(const G4Track& aTrack, 
88                           G4double previousStepSize, 
89                           G4ForceCondition* condition);
90
91private: 
92
93  // Hide copy constructor and assignment operator as private
94  G4PenelopeCompton& operator=(const G4PenelopeCompton& right);
95  G4PenelopeCompton(const G4PenelopeCompton& );
96
97  void ReadData();
98
99  G4double CrossSection(G4double energy,G4int Z);
100  G4double DifferentialCrossSection (G4double cdt);
101
102  G4double lowEnergyLimit;  // low energy limit  applied to the process
103  G4double highEnergyLimit; // high energy limit applied to the process
104
105  G4VEMDataSet* meanFreePathTable;
106  G4VRangeTest* rangeTest;
107
108  const G4double intrinsicLowEnergyLimit; // intrinsic validity range
109  const G4double intrinsicHighEnergyLimit;
110
111  G4double energyForIntegration; //for numerical integration of
112  G4int ZForIntegration;// analytical cross section
113 
114  //Parameters of atomic shells
115  std::map<G4int,G4DataVector*> *ionizationEnergy;
116  std::map<G4int,G4DataVector*> *hartreeFunction;
117  std::map<G4int,G4DataVector*> *occupationNumber;
118
119 
120  G4int SelectRandomAtomForCompton(const G4Material* material,G4double e) const;
121
122  const G4int nBins; //for building cross section table
123
124  std::vector<G4VEMDataSet*> *matCrossSections; //for random choice of atom
125
126  G4double cutForLowEnergySecondaryPhotons;
127  G4bool fUseAtomicDeexcitation;
128};
129
130#endif
131
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